26.01.2015 Views

II II II II II I - Waste Isolation Pilot Plant - U.S. Department of Energy

II II II II II I - Waste Isolation Pilot Plant - U.S. Department of Energy

II II II II II I - Waste Isolation Pilot Plant - U.S. Department of Energy

SHOW MORE
SHOW LESS
  • No tags were found...

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

and assume that the plastic part <strong>of</strong> the strain rate is given by a normality condition<br />

@ . ~<br />

(4.5.9)<br />

when the scalar multiplier,<br />

y, must be determined.<br />

A scalar measure <strong>of</strong> equivalent plastic strain rate is defined by<br />

(4.5.10)<br />

which is chosen<br />

such that<br />

(4.5.11)<br />

The stress rate is assumed to be purely due to the elastic part <strong>of</strong> the strain rate and is expressed in terms <strong>of</strong><br />

Hooke’s law by<br />

d=hrdeb+2pde1 (4.5.12)<br />

where k and ~ are the Lame constants<br />

for the material.<br />

Below, we develop the theory for the cases <strong>of</strong> isotropic hardening, kinematic hardening, and combined<br />

hardening separately so that the reader can see the details for each case.<br />

4.5.1 Isotropic Hardening<br />

In the isotropic hardening case, the backstress is zero and the stress difference is equal to the deviatoric stress, S.<br />

We write a consistency condition by taking the rate <strong>of</strong> Equation (4.5.4)<br />

f(@=2KK . (4.5.13)<br />

By consistency we mean that the state <strong>of</strong> stress must remain on the yield surface at all times. We use the chain rule<br />

and the definition <strong>of</strong> the normal to the yield surface given by Equation (4.5.7) to obtain<br />

af . af<br />

‘(o) ‘Xi:o = z ‘6<br />

(4.5.14)<br />

and from Equations (4.5.3) and (4.5.4)<br />

(4.5.15)<br />

Combining Equations (4.5. 13), (4.5. 14), and (4.5.15)<br />

38

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!